Possible excitonic phase of (Pr1-yRy)1-xCaxCoO3 (R = Lanthanides and Y)
Abstract
(Pr1-yRy)1-xCaxCoO3 (R = Y and/or Lanthanide elements) exhibits a “hidden order transition” in the (x, y) region near (0.5, 0.0) at temperature Ts, where none of magnetic ordering and change of the space group have been found, even though significant anomalies in various physical quantities exist. When the (x, y) is outside of the above region, the transition can essentially be understood by the spin-state-crossover of isolated Co atoms. To study whether excitonic condensation (EC) recently proposed is relevant to the “hidden order transition”, we measured magnetic excitation spectra χ” (Q, ω) by means of inelastic neutron scattering on a single crystal of (Pr0.8Y0.2)0.7Ca0.3CoO3, and obtained following results: While the spectra from the Co 3d electrons observed at 200 K (>above Ts) have characteristics of ordinary strongly correlated electron systems, the χ” (Q, ω) - ω curve at 4 K (<Ts) has a feature reminiscent, at first sight, of a weak pseudogap-like structure. This result can be explained by the realization of the EC phase or “EIQ” phase or at least by the picture that the system is in the boundary region between the low-spin and EQI"phases. Finally, this result strongly suggests that there exists the EIQ phase in themore »
- Authors:
-
- Comprehensive Research Organization for Science and Society (CROSS), Ibaraki (Japan)
- Oak Ridge National Lab. (ORNL), Oak Ridge, TN (United States)
- Nagoya Univ., Nagoya (Japan)
- Publication Date:
- Research Org.:
- Oak Ridge National Lab. (ORNL), Oak Ridge, TN (United States)
- Sponsoring Org.:
- USDOE Office of Science (SC), Basic Energy Sciences (BES)
- OSTI Identifier:
- 1489095
- Grant/Contract Number:
- AC05-00OR22725
- Resource Type:
- Accepted Manuscript
- Journal Name:
- Physica. B, Condensed Matter
- Additional Journal Information:
- Journal Volume: 551; Journal Issue: C; Journal ID: ISSN 0921-4526
- Publisher:
- Elsevier
- Country of Publication:
- United States
- Language:
- English
- Subject:
- 75 CONDENSED MATTER PHYSICS, SUPERCONDUCTIVITY AND SUPERFLUIDITY; Excitonic condensation; Perovskite cobalt oxides; Hidden order; Magnetic excitation spectra; Neutron scattering
Citation Formats
Moyoshi, Taketo, Kamazawa, Kazuya, Matsuda, Masaaki, and Sato, Masatoshi. Possible excitonic phase of (Pr1-yRy)1-xCaxCoO3 (R = Lanthanides and Y). United States: N. p., 2017.
Web. doi:10.1016/j.physb.2017.11.055.
Moyoshi, Taketo, Kamazawa, Kazuya, Matsuda, Masaaki, & Sato, Masatoshi. Possible excitonic phase of (Pr1-yRy)1-xCaxCoO3 (R = Lanthanides and Y). United States. https://doi.org/10.1016/j.physb.2017.11.055
Moyoshi, Taketo, Kamazawa, Kazuya, Matsuda, Masaaki, and Sato, Masatoshi. Thu .
"Possible excitonic phase of (Pr1-yRy)1-xCaxCoO3 (R = Lanthanides and Y)". United States. https://doi.org/10.1016/j.physb.2017.11.055. https://www.osti.gov/servlets/purl/1489095.
@article{osti_1489095,
title = {Possible excitonic phase of (Pr1-yRy)1-xCaxCoO3 (R = Lanthanides and Y)},
author = {Moyoshi, Taketo and Kamazawa, Kazuya and Matsuda, Masaaki and Sato, Masatoshi},
abstractNote = {(Pr1-yRy)1-xCaxCoO3 (R = Y and/or Lanthanide elements) exhibits a “hidden order transition” in the (x, y) region near (0.5, 0.0) at temperature Ts, where none of magnetic ordering and change of the space group have been found, even though significant anomalies in various physical quantities exist. When the (x, y) is outside of the above region, the transition can essentially be understood by the spin-state-crossover of isolated Co atoms. To study whether excitonic condensation (EC) recently proposed is relevant to the “hidden order transition”, we measured magnetic excitation spectra χ” (Q, ω) by means of inelastic neutron scattering on a single crystal of (Pr0.8Y0.2)0.7Ca0.3CoO3, and obtained following results: While the spectra from the Co 3d electrons observed at 200 K (>above Ts) have characteristics of ordinary strongly correlated electron systems, the χ” (Q, ω) - ω curve at 4 K (<Ts) has a feature reminiscent, at first sight, of a weak pseudogap-like structure. This result can be explained by the realization of the EC phase or “EIQ” phase or at least by the picture that the system is in the boundary region between the low-spin and EQI"phases. Finally, this result strongly suggests that there exists the EIQ phase in the present sample or at least in (Pr1–yRy)1–xCaxCoO3 with (x, y) near (0.5, 0.0).},
doi = {10.1016/j.physb.2017.11.055},
journal = {Physica. B, Condensed Matter},
number = C,
volume = 551,
place = {United States},
year = {Thu Nov 23 00:00:00 EST 2017},
month = {Thu Nov 23 00:00:00 EST 2017}
}
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